Номер 49, страница 91 - гдз по физике 10-11 класс задачник Гельфгат, Генденштейн

Физика, 10-11 класс Задачник, авторы: Гельфгат Илья Маркович, Генденштейн Лев Элевич, Кирик Леонид Анатольевич, издательство Илекса, Москва, 2008, красного цвета

Авторы: Гельфгат И. М., Генденштейн Л. Э., Кирик Л. А.

Тип: Задачник

Издательство: Илекса

Год издания: 2008 - 2026

Уровень обучения: профильный

Цвет обложки: красный лупа, парень едет на велосипеде

ISBN: 978-5-89237-252-7

Механика. Механические колебания и волны. 12. Механические колебания. Олимпиадные задачи - номер 49, страница 91.

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            "field_h1" => null
            "field_description_top" => null
            "field_description_bottom" => null
            "field_branch_cover" => []
            "field_branch_covers" => []
            "book" => Illuminate\Database\Eloquent\Collection {#1073}
            "branch_parent" => Illuminate\Database\Eloquent\Collection {#1107}
          ]
          #changes: []
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          #classCastCache: []
          #attributeCastCache: []
          #dateFormat: null
          #appends: []
          #dispatchesEvents: []
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          #touches: []
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          #hidden: []
          #visible: []
          #fillable: []
          #guarded: array:1 [
            0 => "*"
          ]
        }
        1 => App\Models\Branch {#1108
          #connection: "mysql"
          #table: "branches"
          #primaryKey: "id"
          #keyType: "int"
          +incrementing: true
          #with: []
          #withCount: []
          +preventsLazyLoading: false
          #perPage: 15
          +exists: true
          +wasRecentlyCreated: false
          #escapeWhenCastingToString: false
          #attributes: array:24 [
            "id" => 1319303
            "created_at" => "2026-04-10 13:58:26"
            "updated_at" => null
            "field_display_title" => "Механические колебания и волны"
            "field_branch_order" => null
            "field_url" => null
            "field_branch_type" => Illuminate\Database\Eloquent\Collection {#1109
              #items: []
              #escapeWhenCastingToString: false
            }
            "field_page_start" => "88"
            "field_branch_display" => "0"
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            "field_display_branch_in_title" => "1"
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            "field_navigation_title" => null
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            "field_metatags_description" => null
            "field_h1" => null
            "field_description_top" => null
            "field_description_bottom" => null
            "field_branch_cover" => []
            "field_branch_covers" => []
            "book" => Illuminate\Database\Eloquent\Collection {#1110
              #items: array:1 [
                0 => App\Models\Book {#1111
                  #connection: "mysql"
                  #table: "books"
                  #primaryKey: "id"
                  #keyType: "int"
                  +incrementing: false
                  #with: []
                  #withCount: []
                  +preventsLazyLoading: false
                  #perPage: 15
                  +exists: true
                  +wasRecentlyCreated: false
                  #escapeWhenCastingToString: false
                  #attributes: array:50 [
                    "id" => 5400
                    "created_at" => "2026-04-10 13:58:26"
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                    "field_subject" => Illuminate\Database\Eloquent\Collection {#1112 …2}
                    "field_class" => Illuminate\Database\Eloquent\Collection {#1114 …2}
                    "field_publisher" => Illuminate\Database\Eloquent\Collection {#1117 …2}
                    "field_author" => Illuminate\Database\Eloquent\Collection {#1119 …2}
                    "field_author_foreign" => Illuminate\Database\Eloquent\Collection {#1123 …2}
                    "field_book_type" => Illuminate\Database\Eloquent\Collection {#1124 …2}
                    "field_country" => Illuminate\Database\Eloquent\Collection {#1126 …2}
                    "field_city" => Illuminate\Database\Eloquent\Collection {#1128 …2}
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                    "field_level_of_education" => Illuminate\Database\Eloquent\Collection {#1132 …2}
                    "field_standart_of_education" => Illuminate\Database\Eloquent\Collection {#1134 …2}
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                    "field_publication_type" => Illuminate\Database\Eloquent\Collection {#1135 …2}
                    "field_under_the_edition" => Illuminate\Database\Eloquent\Collection {#1136 …2}
                    "field_under_the_edition_degree" => null
                    "field_cover_description" => "лупа, парень едет на велосипеде"
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                    "field_default_folder" => "/fizika_10/gelfgat-z/"
                    "field_isbn" => "978-5-89237-252-7"
                    "field_cover" => array:1 [ …1]
                    "field_cover_alts" => array:1 [ …1]
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                    "breadcrumbs" => array:3 [ …3]
                  ]
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                    "id" => 5400
                    "created_at" => "2026-04-10 13:58:26"
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                    "field_author_foreign" => Illuminate\Database\Eloquent\Collection {#1123 …2}
                    "field_book_type" => Illuminate\Database\Eloquent\Collection {#1124 …2}
                    "field_country" => Illuminate\Database\Eloquent\Collection {#1126 …2}
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                    "field_standart_of_education" => Illuminate\Database\Eloquent\Collection {#1134 …2}
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                    "field_under_the_edition" => Illuminate\Database\Eloquent\Collection {#1136 …2}
                    "field_under_the_edition_degree" => null
                    "field_cover_description" => "лупа, парень едет на велосипеде"
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                    "field_default_folder" => "/fizika_10/gelfgat-z/"
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                    "field_cover" => array:1 [ …1]
                    "field_cover_alts" => array:1 [ …1]
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                    "breadcrumbs" => array:3 [ …3]
                  ]
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                    0 => "*"
                  ]
                }
              ]
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            }
            "branch_parent" => Illuminate\Database\Eloquent\Collection {#1142
              #items: array:1 [
                0 => App\Models\Branch {#1143
                  #connection: "mysql"
                  #table: "branches"
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                  #keyType: "int"
                  +incrementing: true
                  #with: []
                  #withCount: []
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                  #perPage: 15
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                  +wasRecentlyCreated: false
                  #escapeWhenCastingToString: false
                  #attributes: array:24 [
                    "id" => 1319266
                    "created_at" => "2026-04-10 13:58:26"
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                    "book" => Illuminate\Database\Eloquent\Collection {#1145 …2}
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                  ]
                  #original: array:24 [
                    "id" => 1319266
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                    "updated_at" => null
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                    "field_branch_type" => Illuminate\Database\Eloquent\Collection {#1144 …2}
                    "field_page_start" => "6"
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                    "book" => Illuminate\Database\Eloquent\Collection {#1145 …2}
                    "branch_parent" => Illuminate\Database\Eloquent\Collection {#1146 …2}
                  ]
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                  #touches: []
                  +timestamps: true
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                  #hidden: []
                  #visible: []
                  #fillable: []
                  #guarded: array:1 [
                    0 => "*"
                  ]
                }
              ]
              #escapeWhenCastingToString: false
            }
          ]
          #original: array:24 [
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            "created_at" => "2026-04-10 13:58:26"
            "updated_at" => null
            "field_display_title" => "Механические колебания и волны"
            "field_branch_order" => null
            "field_url" => null
            "field_branch_type" => Illuminate\Database\Eloquent\Collection {#1109}
            "field_page_start" => "88"
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            "field_h1" => null
            "field_description_top" => null
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            "field_branch_cover" => []
            "field_branch_covers" => []
            "book" => Illuminate\Database\Eloquent\Collection {#1110}
            "branch_parent" => Illuminate\Database\Eloquent\Collection {#1142}
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          #changes: []
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          #attributeCastCache: []
          #dateFormat: null
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          #touches: []
          +timestamps: true
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          #hidden: []
          #visible: []
          #fillable: []
          #guarded: array:1 [
            0 => "*"
          ]
        }
        2 => App\Models\Branch {#1147
          #connection: "mysql"
          #table: "branches"
          #primaryKey: "id"
          #keyType: "int"
          +incrementing: true
          #with: []
          #withCount: []
          +preventsLazyLoading: false
          #perPage: 15
          +exists: true
          +wasRecentlyCreated: false
          #escapeWhenCastingToString: false
          #attributes: array:24 [
            "id" => 1319304
            "created_at" => "2026-04-10 13:58:26"
            "updated_at" => null
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            "field_branch_order" => null
            "field_url" => null
            "field_branch_type" => Illuminate\Database\Eloquent\Collection {#1148
              #items: []
              #escapeWhenCastingToString: false
            }
            "field_page_start" => "88"
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            "field_h1" => null
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            "field_branch_cover" => []
            "field_branch_covers" => []
            "book" => Illuminate\Database\Eloquent\Collection {#1149
              #items: array:1 [
                0 => App\Models\Book {#1150
                  #connection: "mysql"
                  #table: "books"
                  #primaryKey: "id"
                  #keyType: "int"
                  +incrementing: false
                  #with: []
                  #withCount: []
                  +preventsLazyLoading: false
                  #perPage: 15
                  +exists: true
                  +wasRecentlyCreated: false
                  #escapeWhenCastingToString: false
                  #attributes: array:50 [
                    "id" => 5400
                    "created_at" => "2026-04-10 13:58:26"
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                    "field_subject" => Illuminate\Database\Eloquent\Collection {#1151 …2}
                    "field_class" => Illuminate\Database\Eloquent\Collection {#1153 …2}
                    "field_publisher" => Illuminate\Database\Eloquent\Collection {#1156 …2}
                    "field_author" => Illuminate\Database\Eloquent\Collection {#1158 …2}
                    "field_author_foreign" => Illuminate\Database\Eloquent\Collection {#1162 …2}
                    "field_book_type" => Illuminate\Database\Eloquent\Collection {#1163 …2}
                    "field_country" => Illuminate\Database\Eloquent\Collection {#1165 …2}
                    "field_city" => Illuminate\Database\Eloquent\Collection {#1167 …2}
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                    "field_level_of_education" => Illuminate\Database\Eloquent\Collection {#1171 …2}
                    "field_standart_of_education" => Illuminate\Database\Eloquent\Collection {#1173 …2}
                    "field_publication_number" => null
                    "field_publication_type" => Illuminate\Database\Eloquent\Collection {#1174 …2}
                    "field_under_the_edition" => Illuminate\Database\Eloquent\Collection {#1175 …2}
                    "field_under_the_edition_degree" => null
                    "field_cover_description" => "лупа, парень едет на велосипеде"
                    "field_publication_year" => "2008"
                    "field_publication_year_until" => null
                    "field_part" => ""
                    "field_part_writing" => ""
                    "field_second_foreign_language" => null
                    "field_for_whom" => "Учебное издание"
                    "field_allowed" => null
                    "field_reserve_field" => null
                    "field_link_to_source" => null
                    "field_tasks_count" => "459"
                    "field_priority" => null
                    "field_default_folder" => "/fizika_10/gelfgat-z/"
                    "field_isbn" => "978-5-89237-252-7"
                    "field_cover" => array:1 [ …1]
                    "field_cover_alts" => array:1 [ …1]
                    "field_covers" => array:1 [ …1]
                    "field_popular_book" => "0"
                    "field_recommended_books" => Illuminate\Database\Eloquent\Collection {#1176 …2}
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                    "field_url" => "/10-klass/fizika/gelfgat-zadachnik"
                    "field_cover_color" => Illuminate\Database\Eloquent\Collection {#1179 …2}
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                    "breadcrumbs" => array:3 [ …3]
                  ]
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                    "field_cover_description" => "лупа, парень едет на велосипеде"
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                    "field_cover" => array:1 [ …1]
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                    "field_cover_color" => Illuminate\Database\Eloquent\Collection {#1179 …2}
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                    "breadcrumbs" => array:3 [ …3]
                  ]
                  #changes: []
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                    0 => "*"
                  ]
                }
              ]
              #escapeWhenCastingToString: false
            }
            "branch_parent" => Illuminate\Database\Eloquent\Collection {#1181
              #items: array:1 [
                0 => App\Models\Branch {#1182
                  #connection: "mysql"
                  #table: "branches"
                  #primaryKey: "id"
                  #keyType: "int"
                  +incrementing: true
                  #with: []
                  #withCount: []
                  +preventsLazyLoading: false
                  #perPage: 15
                  +exists: true
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                  #escapeWhenCastingToString: false
                  #attributes: array:24 [
                    "id" => 1319303
                    "created_at" => "2026-04-10 13:58:26"
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                    "field_branch_type" => Illuminate\Database\Eloquent\Collection {#1183 …2}
                    "field_page_start" => "88"
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                    "field_branch_cover" => []
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            "text" => "<p><strong>O-49.</strong> На два быстро вращающихся одинаковых валика положили горизонтально доску массой $\text{m}$ (см. рисунок). Расстояние между осями валиков $\text{L}$, коэффициент трения между доской и валиками $\mu$. Как будет двигаться доска?</p><p>Как изменится ответ, если оба валика изменят направление вращения?</p><p>&#9745; Доска будет совершать гармонические колебания с периодом $T = 2\pi\sqrt{L/(2\mu g)}$. Если валики изменят направление вращения, доска будет сброшена с них.</p><p><strong>Решение.</strong> В условии говорится о быстром вращении валиков; значит, между ними и доской действуют силы трения скольжения (см. рисунок).</p><p>Следовательно, $ma_x = F_{тр1} - F_{тр2} = \mu(N_1 - N_2)$, где $N_1$ и $N_2$ — силы давления доски на первый и второй валики. В положении равновесия центр доски C расположен на равных расстояниях от обоих валиков. Если доска сместилась от положения равновесия на расстояние $\text{x}$, то $\frac{N_1}{N_2} = \frac{0,5L - x}{0,5L + x}$.</p><p>Учитывая, что $N_1 + N_2 = mg$, получаем: $N_1 = mg(1/2 - x/L)$ и $N_2 = mg(1/2 + x/L)$.</p><p>Уравнение движения принимает вид $a_x = -(2\mu g/L)x$. Это уравнение гармонических колебаний с циклической частотой $\omega_0 = \sqrt{2\mu g/L}$ и периодом $T = 2\pi\sqrt{L/(2\mu g)}$.</p><p>Если валики изменят направление вращения, то обе силы трения будут направлены «наружу». Смещение доски от положения равновесия увеличит на этот раз ту силу трения, которая стремится увеличить смещение. Следовательно, равновесие в этом случае неустойчиво: доска будет сброшена с валиков.</p>"
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            "text" => "<p><strong>O-49.</strong> На два быстро вращающихся одинаковых валика положили горизонтально доску массой $\text{m}$ (см. рисунок). Расстояние между осями валиков $\text{L}$, коэффициент трения между доской и валиками $\mu$. Как будет двигаться доска?</p><p>Как изменится ответ, если оба валика изменят направление вращения?</p><p>&#9745; Доска будет совершать гармонические колебания с периодом $T = 2\pi\sqrt{L/(2\mu g)}$. Если валики изменят направление вращения, доска будет сброшена с них.</p><p><strong>Решение.</strong> В условии говорится о быстром вращении валиков; значит, между ними и доской действуют силы трения скольжения (см. рисунок).</p><p>Следовательно, $ma_x = F_{тр1} - F_{тр2} = \mu(N_1 - N_2)$, где $N_1$ и $N_2$ — силы давления доски на первый и второй валики. В положении равновесия центр доски C расположен на равных расстояниях от обоих валиков. Если доска сместилась от положения равновесия на расстояние $\text{x}$, то $\frac{N_1}{N_2} = \frac{0,5L - x}{0,5L + x}$.</p><p>Учитывая, что $N_1 + N_2 = mg$, получаем: $N_1 = mg(1/2 - x/L)$ и $N_2 = mg(1/2 + x/L)$.</p><p>Уравнение движения принимает вид $a_x = -(2\mu g/L)x$. Это уравнение гармонических колебаний с циклической частотой $\omega_0 = \sqrt{2\mu g/L}$ и периодом $T = 2\pi\sqrt{L/(2\mu g)}$.</p><p>Если валики изменят направление вращения, то обе силы трения будут направлены «наружу». Смещение доски от положения равновесия увеличит на этот раз ту силу трения, которая стремится увеличить смещение. Следовательно, равновесие в этом случае неустойчиво: доска будет сброшена с валиков.</p>"
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            "text" => "<p><strong>Дано:</strong></p><p>масса доски: $m$</p><p>расстояние между осями валиков: $L$</p><p>коэффициент трения скольжения: $μ$</p><p>ускорение свободного падения: $g$</p><p><strong>Найти:</strong></p><p><strong>1.</strong> Как будет двигаться доска.</p><p><strong>2.</strong> Как изменится характер движения, если валики изменят направление вращения.</p><p><strong>Решение:</strong></p><p><strong>Как будет двигаться доска?</strong></p><p>По умолчанию будем считать, что валики вращаются "внутрь", то есть их верхние поверхности движутся навстречу друг другу. Введем горизонтальную ось $Ox$, начало которой ($x=0$) находится ровно посередине между валиками.</p><p>Рассмотрим доску, смещенную из положения равновесия вправо на расстояние $x$. На доску действуют вертикальные силы: сила тяжести $mg$ и силы нормальной реакции опор $N_1$ (левый валик) и $N_2$ (правый валик). Из условия равновесия по вертикали:</p><p>$N_1 + N_2 = mg$</p><p>Для нахождения $N_1$ и $N_2$ по отдельности запишем уравнение моментов относительно центра масс доски C (который находится в точке $x$). Расстояние от центра масс до левого валика равно $L/2 + x$, а до правого $L/2 - x$.</p><p>$N_1(L/2 + x) - N_2(L/2 - x) = 0$</p><p>Решая эту систему уравнений, получаем:</p><p>$N_1 = mg(\frac{1}{2} - \frac{x}{L})$</p><p>$N_2 = mg(\frac{1}{2} + \frac{x}{L})$</p><p>При вращении валиков "внутрь" сила трения от левого валика $F_{тр1}$ направлена вправо, а от правого валика $F_{тр2}$ — влево. Результирующая сила, действующая на доску в горизонтальном направлении, равна:</p><p>$F_x = F_{тр1} - F_{тр2} = μN_1 - μN_2$</p><p>Подставим выражения для $N_1$ и $N_2$:</p><p>$F_x = μ[mg(\frac{1}{2} - \frac{x}{L}) - mg(\frac{1}{2} + \frac{x}{L})] = μmg(-\frac{2x}{L}) = -(\frac{2μmg}{L})x$</p><p>Согласно второму закону Ньютона, $F_x = ma_x$.</p><p>$ma_x = -(\frac{2μmg}{L})x$</p><p>Сокращая массу $m$, получаем уравнение для ускорения:</p><p>$a_x = -(\frac{2μg}{L})x$</p><p>Это уравнение описывает гармонические колебания вида $a_x = -ω^2x$. Отсюда можно найти циклическую частоту колебаний $ω$:</p><p>$ω^2 = \frac{2μg}{L} \implies ω = \sqrt{\frac{2μg}{L}}$</p><p>Период колебаний $T$ связан с циклической частотой как $T = 2π/ω$.</p><p>$T = 2π\sqrt{\frac{L}{2μg}}$</p><p>Таким образом, доска будет совершать незатухающие гармонические колебания около положения равновесия.</p><p><strong>Ответ:</strong> Доска будет совершать гармонические колебания с периодом $T = 2π\sqrt{\frac{L}{2μg}}$.</p><p><strong>Как изменится ответ, если оба валика изменят направление вращения?</strong></p><p>Если валики начнут вращаться "наружу", то направления сил трения изменятся на противоположные. Сила трения от левого валика $F_{тр1}$ будет направлена влево, а от правого $F_{тр2}$ — вправо.</p><p>Снова сместим доску вправо на расстояние $x$. Результирующая сила будет равна:</p><p>$F_x = F_{тр2} - F_{тр1} = μN_2 - μN_1$</p><p>Подставим выражения для $N_1$ и $N_2$:</p><p>$F_x = μ[mg(\frac{1}{2} + \frac{x}{L}) - mg(\frac{1}{2} - \frac{x}{L})] = μmg(\frac{2x}{L}) = +(\frac{2μmg}{L})x$</p><p>Уравнение движения примет вид:</p><p>$a_x = +(\frac{2μg}{L})x$</p><p>В этом случае результирующая сила направлена в ту же сторону, что и смещение. Такая сила не возвращает тело в положение равновесия, а наоборот, увеличивает его смещение. Положение равновесия $x=0$ становится неустойчивым. Любое случайное смещение будет нарастать, и доска будет сброшена с валиков.</p><p><strong>Ответ:</strong> Положение равновесия станет неустойчивым. При малейшем смещении от центра доска начнет ускоренно двигаться в сторону смещения и в итоге будет сброшена с валиков.</p>"
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            "text" => "<p><strong>Дано:</strong></p><p>масса доски: $m$</p><p>расстояние между осями валиков: $L$</p><p>коэффициент трения скольжения: $μ$</p><p>ускорение свободного падения: $g$</p><p><strong>Найти:</strong></p><p><strong>1.</strong> Как будет двигаться доска.</p><p><strong>2.</strong> Как изменится характер движения, если валики изменят направление вращения.</p><p><strong>Решение:</strong></p><p><strong>Как будет двигаться доска?</strong></p><p>По умолчанию будем считать, что валики вращаются "внутрь", то есть их верхние поверхности движутся навстречу друг другу. Введем горизонтальную ось $Ox$, начало которой ($x=0$) находится ровно посередине между валиками.</p><p>Рассмотрим доску, смещенную из положения равновесия вправо на расстояние $x$. На доску действуют вертикальные силы: сила тяжести $mg$ и силы нормальной реакции опор $N_1$ (левый валик) и $N_2$ (правый валик). Из условия равновесия по вертикали:</p><p>$N_1 + N_2 = mg$</p><p>Для нахождения $N_1$ и $N_2$ по отдельности запишем уравнение моментов относительно центра масс доски C (который находится в точке $x$). Расстояние от центра масс до левого валика равно $L/2 + x$, а до правого $L/2 - x$.</p><p>$N_1(L/2 + x) - N_2(L/2 - x) = 0$</p><p>Решая эту систему уравнений, получаем:</p><p>$N_1 = mg(\frac{1}{2} - \frac{x}{L})$</p><p>$N_2 = mg(\frac{1}{2} + \frac{x}{L})$</p><p>При вращении валиков "внутрь" сила трения от левого валика $F_{тр1}$ направлена вправо, а от правого валика $F_{тр2}$ — влево. Результирующая сила, действующая на доску в горизонтальном направлении, равна:</p><p>$F_x = F_{тр1} - F_{тр2} = μN_1 - μN_2$</p><p>Подставим выражения для $N_1$ и $N_2$:</p><p>$F_x = μ[mg(\frac{1}{2} - \frac{x}{L}) - mg(\frac{1}{2} + \frac{x}{L})] = μmg(-\frac{2x}{L}) = -(\frac{2μmg}{L})x$</p><p>Согласно второму закону Ньютона, $F_x = ma_x$.</p><p>$ma_x = -(\frac{2μmg}{L})x$</p><p>Сокращая массу $m$, получаем уравнение для ускорения:</p><p>$a_x = -(\frac{2μg}{L})x$</p><p>Это уравнение описывает гармонические колебания вида $a_x = -ω^2x$. Отсюда можно найти циклическую частоту колебаний $ω$:</p><p>$ω^2 = \frac{2μg}{L} \implies ω = \sqrt{\frac{2μg}{L}}$</p><p>Период колебаний $T$ связан с циклической частотой как $T = 2π/ω$.</p><p>$T = 2π\sqrt{\frac{L}{2μg}}$</p><p>Таким образом, доска будет совершать незатухающие гармонические колебания около положения равновесия.</p><p><strong>Ответ:</strong> Доска будет совершать гармонические колебания с периодом $T = 2π\sqrt{\frac{L}{2μg}}$.</p><p><strong>Как изменится ответ, если оба валика изменят направление вращения?</strong></p><p>Если валики начнут вращаться "наружу", то направления сил трения изменятся на противоположные. Сила трения от левого валика $F_{тр1}$ будет направлена влево, а от правого $F_{тр2}$ — вправо.</p><p>Снова сместим доску вправо на расстояние $x$. Результирующая сила будет равна:</p><p>$F_x = F_{тр2} - F_{тр1} = μN_2 - μN_1$</p><p>Подставим выражения для $N_1$ и $N_2$:</p><p>$F_x = μ[mg(\frac{1}{2} + \frac{x}{L}) - mg(\frac{1}{2} - \frac{x}{L})] = μmg(\frac{2x}{L}) = +(\frac{2μmg}{L})x$</p><p>Уравнение движения примет вид:</p><p>$a_x = +(\frac{2μg}{L})x$</p><p>В этом случае результирующая сила направлена в ту же сторону, что и смещение. Такая сила не возвращает тело в положение равновесия, а наоборот, увеличивает его смещение. Положение равновесия $x=0$ становится неустойчивым. Любое случайное смещение будет нарастать, и доска будет сброшена с валиков.</p><p><strong>Ответ:</strong> Положение равновесия станет неустойчивым. При малейшем смещении от центра доска начнет ускоренно двигаться в сторону смещения и в итоге будет сброшена с валиков.</p>"
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                }
                1 => App\Models\Term {#1327
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                  #table: "terms"
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                  #keyType: "int"
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                }
                2 => App\Models\Term {#1328
                  #connection: "mysql"
                  #table: "terms"
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                  #keyType: "int"
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                }
              ]
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            }
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              #escapeWhenCastingToString: false
            }
            "field_book_type" => Illuminate\Database\Eloquent\Collection {#1330
              #items: array:1 [
                0 => App\Models\Term {#1331
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                  #table: "terms"
                  #primaryKey: "id"
                  #keyType: "int"
                  +incrementing: false
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                }
              ]
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            "field_country" => Illuminate\Database\Eloquent\Collection {#1332
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                0 => App\Models\Term {#1333
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                }
              ]
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            }
            "field_city" => Illuminate\Database\Eloquent\Collection {#1334
              #items: array:1 [
                0 => App\Models\Term {#1335
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                  #table: "terms"
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              ]
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            "field_level_of_education" => Illuminate\Database\Eloquent\Collection {#1338
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                0 => App\Models\Term {#1339
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              ]
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      ]
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    }
    "page" => Illuminate\Database\Eloquent\Collection {#1355
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        0 => App\Models\BookPage {#1354
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            }
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            }
            "content" => Illuminate\Database\Eloquent\Collection {#1368
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                0 => App\Models\Element {#1367
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                }
              ]
              #escapeWhenCastingToString: false
            }
            "next" => array:2 [
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            ]
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            "tasks" => Illuminate\Database\Eloquent\Collection {#1984
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                0 => App\Models\Task {#1360
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                  #primaryKey: "id"
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                }
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                }
                2 => App\Models\Task {#1667
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              ]
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          ]
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            "field_metatags_description" => null
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            "field_description_bottom" => null
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            "content" => Illuminate\Database\Eloquent\Collection {#1368}
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          ]
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      ]
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  ]
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}
№49 (с. 91)
Условие. №49 (с. 91)
скриншот условия
Физика, 10-11 класс Задачник, авторы: Гельфгат Илья Маркович, Генденштейн Лев Элевич, Кирик Леонид Анатольевич, издательство Илекса, Москва, 2008, красного цвета, страница 91, номер 49, Условие
Физика, 10-11 класс Задачник, авторы: Гельфгат Илья Маркович, Генденштейн Лев Элевич, Кирик Леонид Анатольевич, издательство Илекса, Москва, 2008, красного цвета, страница 91, номер 49, Условие (продолжение 2)

O-49. На два быстро вращающихся одинаковых валика положили горизонтально доску массой $\text{m}$ (см. рисунок). Расстояние между осями валиков $\text{L}$, коэффициент трения между доской и валиками $\mu$. Как будет двигаться доска?

Как изменится ответ, если оба валика изменят направление вращения?

☑ Доска будет совершать гармонические колебания с периодом $T = 2\pi\sqrt{L/(2\mu g)}$. Если валики изменят направление вращения, доска будет сброшена с них.

Решение. В условии говорится о быстром вращении валиков; значит, между ними и доской действуют силы трения скольжения (см. рисунок).

Следовательно, $ma_x = F_{тр1} - F_{тр2} = \mu(N_1 - N_2)$, где $N_1$ и $N_2$ — силы давления доски на первый и второй валики. В положении равновесия центр доски C расположен на равных расстояниях от обоих валиков. Если доска сместилась от положения равновесия на расстояние $\text{x}$, то $\frac{N_1}{N_2} = \frac{0,5L - x}{0,5L + x}$.

Учитывая, что $N_1 + N_2 = mg$, получаем: $N_1 = mg(1/2 - x/L)$ и $N_2 = mg(1/2 + x/L)$.

Уравнение движения принимает вид $a_x = -(2\mu g/L)x$. Это уравнение гармонических колебаний с циклической частотой $\omega_0 = \sqrt{2\mu g/L}$ и периодом $T = 2\pi\sqrt{L/(2\mu g)}$.

Если валики изменят направление вращения, то обе силы трения будут направлены «наружу». Смещение доски от положения равновесия увеличит на этот раз ту силу трения, которая стремится увеличить смещение. Следовательно, равновесие в этом случае неустойчиво: доска будет сброшена с валиков.

Решение. №49 (с. 91)

Дано:

масса доски: $m$

расстояние между осями валиков: $L$

коэффициент трения скольжения: $μ$

ускорение свободного падения: $g$

Найти:

1. Как будет двигаться доска.

2. Как изменится характер движения, если валики изменят направление вращения.

Решение:

Как будет двигаться доска?

По умолчанию будем считать, что валики вращаются "внутрь", то есть их верхние поверхности движутся навстречу друг другу. Введем горизонтальную ось $Ox$, начало которой ($x=0$) находится ровно посередине между валиками.

Рассмотрим доску, смещенную из положения равновесия вправо на расстояние $x$. На доску действуют вертикальные силы: сила тяжести $mg$ и силы нормальной реакции опор $N_1$ (левый валик) и $N_2$ (правый валик). Из условия равновесия по вертикали:

$N_1 + N_2 = mg$

Для нахождения $N_1$ и $N_2$ по отдельности запишем уравнение моментов относительно центра масс доски C (который находится в точке $x$). Расстояние от центра масс до левого валика равно $L/2 + x$, а до правого $L/2 - x$.

$N_1(L/2 + x) - N_2(L/2 - x) = 0$

Решая эту систему уравнений, получаем:

$N_1 = mg(\frac{1}{2} - \frac{x}{L})$

$N_2 = mg(\frac{1}{2} + \frac{x}{L})$

При вращении валиков "внутрь" сила трения от левого валика $F_{тр1}$ направлена вправо, а от правого валика $F_{тр2}$ — влево. Результирующая сила, действующая на доску в горизонтальном направлении, равна:

$F_x = F_{тр1} - F_{тр2} = μN_1 - μN_2$

Подставим выражения для $N_1$ и $N_2$:

$F_x = μ[mg(\frac{1}{2} - \frac{x}{L}) - mg(\frac{1}{2} + \frac{x}{L})] = μmg(-\frac{2x}{L}) = -(\frac{2μmg}{L})x$

Согласно второму закону Ньютона, $F_x = ma_x$.

$ma_x = -(\frac{2μmg}{L})x$

Сокращая массу $m$, получаем уравнение для ускорения:

$a_x = -(\frac{2μg}{L})x$

Это уравнение описывает гармонические колебания вида $a_x = -ω^2x$. Отсюда можно найти циклическую частоту колебаний $ω$:

$ω^2 = \frac{2μg}{L} \implies ω = \sqrt{\frac{2μg}{L}}$

Период колебаний $T$ связан с циклической частотой как $T = 2π/ω$.

$T = 2π\sqrt{\frac{L}{2μg}}$

Таким образом, доска будет совершать незатухающие гармонические колебания около положения равновесия.

Ответ: Доска будет совершать гармонические колебания с периодом $T = 2π\sqrt{\frac{L}{2μg}}$.

Как изменится ответ, если оба валика изменят направление вращения?

Если валики начнут вращаться "наружу", то направления сил трения изменятся на противоположные. Сила трения от левого валика $F_{тр1}$ будет направлена влево, а от правого $F_{тр2}$ — вправо.

Снова сместим доску вправо на расстояние $x$. Результирующая сила будет равна:

$F_x = F_{тр2} - F_{тр1} = μN_2 - μN_1$

Подставим выражения для $N_1$ и $N_2$:

$F_x = μ[mg(\frac{1}{2} + \frac{x}{L}) - mg(\frac{1}{2} - \frac{x}{L})] = μmg(\frac{2x}{L}) = +(\frac{2μmg}{L})x$

Уравнение движения примет вид:

$a_x = +(\frac{2μg}{L})x$

В этом случае результирующая сила направлена в ту же сторону, что и смещение. Такая сила не возвращает тело в положение равновесия, а наоборот, увеличивает его смещение. Положение равновесия $x=0$ становится неустойчивым. Любое случайное смещение будет нарастать, и доска будет сброшена с валиков.

Ответ: Положение равновесия станет неустойчивым. При малейшем смещении от центра доска начнет ускоренно двигаться в сторону смещения и в итоге будет сброшена с валиков.

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